Self-collimator concave spectra shaping device for chirped-pulse-amplification

ABSTRACT

A self-collimator concave spectral shaping device for chirped-pulse-amplification (CPA): uses a spectrum decomposing system with CTSI construction, a spectrum synthesizing system with CTSI structure that is symmetrical to the decomposing structure, and a spectrum shaping system including an aperture and a planar reflector for spectrum shaping function design. The device accomplishes the following functions: firstly decomposing the spectrum of a chirped temporal pulse laser to a spectral domain; then shaping the spectrum in the spectral domain; finally synthesizing un-shiftily this shaped spectrum in the spectral domain into a temporal chirped pulse with a designed shape. The device has the feature of requiring less optical components, compacting the structure, requiring less space, cheap in cost, and running stability, for its small size of concave reflector, and its self-collimation and its symmetrical distribution, which it can be not only utilized in a general laser spectrum shaping and spectrum modulation, but also can be utilized for a high energy and ultra-high peak-power laser system in chirped pulse amplification with a large caliber and with a chirped pulse bandwidth of a few nanometers.

PRIORITY CLAIM

The application titled as a self-collimator concave spectral shaping device for chirped pulse amplification is the international application, PCT/IB2009/050913, filed on 3 May 2009, for entry into the national stage in the United States, where it claims the benefit of the international filing date of the international application designating the United States of America.

TECHNICAL FIELD OF THE INVENTION

The present invention relates generally to a pulse shaping device for laser amplification in the power. The invention related in particular to manipulating the spectral and temporal characteristics of laser pulses, which the self-collimator concave spectral shaping device is for a large caliber and high power chirped pulse amplification (CPA) in huge energy, which belongs to the filed of application technology of engineering optics.

DISCUSSION OF BACKGROUND ART

In the field of the high-power ultra-short laser pulse amplification, the enhancement of the output of a laser system is hampered by a series of factors such as the gain narrowing effect and the gain saturation effect in the solid-state laser amplification medium. The gain narrowing effect is caused by the limited bandwidth of the atomic emission in the laser medium and the frequency pulling effect, which makes the spectrum of the output pulse narrowing that not only leads to the deformity of the pulse waveform but also conducts the chirped pulse hard to be compressed into the original width. The gain saturation effect is another main factor leading to the distortion of CPA. It is caused by the pulse head depletion more the population inversion in the amplification medium than the pulse tail, which leads to the intensity of the pulse head getting more amplification than the intensity of the pulse tail. Hence the output of amplified pulse becomes asymmetric in the pulse waveform, which leads to the lose of amplification efficiency of chirped pulse, which leads to the red shift effect in the spectrum of the laser pulse, and which leads to the distortion of CPA. In order to compensate the gain narrowing and gain saturation effects of CPA, and also to improve the signal to noise ratio (SNR) of the output high-power laser pulse, people needs a kind of spectrum modulation device to shape the spectrum distribution of pre-amplification pulse making it depression in the vicinity of center wavelength in some shapes and in some depths practically. In the inertial confinement fusion (ICF) field, the physics experiments have harsh requirements on the pulse parameter of the output laser. And lots of attention have been paid to the spatial distribution, the temporal profile, as well as the spectrum shaping in the design of kilojoules peta-watt-class laser system, in order to compensate the gain narrowing and gain saturation effects of CPA, and also to improve the SNR of the output high-power laser pulse, such as in the literatures: [X L Chu, B Zhang, B W Cai, et. al., “Study of the Multipass Amplification of the Chirped Pulse and Its Inverse Problem”, Acta Phys. Sin., 2005, 54(10), 4696-1701], [B Zhang, B D Lü, “An Inverse Problem of Multistage and Multipass Pulsed Laser Amplifiers”, Chin. J. Lasers, 1997, 24(6), 495-500], [T Wang, D Y Fan, “Pulse Shaping Design of High Power Laser Amplifier”, High Power Laser and Particle Beams, 1999, 11(2), 139-142], and [X J Huang, X F Wei, H S Peng et. al. “On Structure of a Hundred Terawatt Class Ultra-short Laser System”, 2004, the conference of optoelectronics in Sichuan].

The above literatures also illustrate some defects in the traditional shaping devices, just as following: 1. Using the thin etalon in regenerative amplification to tune the spectrum of the laser pulse, but it is complexity of the device regulation, in addition, a optical parametric chirped pulse amplifier (OPCPA) has substituted the regenerative amplifier in the front-end of kilojoules peta-watt-class laser system, so this method does not apply. 2. Using the center wavelength blue shift injection, that is, making the centre of the pulse wavelength blue shift relative to the centre wavelength of the medium spontaneous emission, making the long wavelength parts of the pulse with a large duration, and making the spectrum modulation directly, but it is not practical to a over terawatt (10¹²) system. 3. Using the long-wavelength injection method that utilizes narrowing effect to compensate saturation effect, but this will make the system unstable. 4. Using the acousto-optic programmable dispersive filter (AOPDF) to compensate the spectral gain narrowing, but it has lower sufferance of the high power laser damages. Although it is equipped with a strong capability of gain compensation and dispersion compensation, it gets success just on the structure of a hundred terawatt class ultra-short laser system but not for the Nd:glass systems.

At the same time, all the transmitted elements such as the optical filter and the birefringent crystal, and all the organic selection elements such as the hinged organic polymer used for modulating the spectrum of the laser pulse, are unusable for the high-power and huge-energy laser, such as in the literatures [P F Zhu, J X Yang, S L Xue, M R Li, Z Q Lin, “Spectrum Shaping of the Ultrashort Pulse”, CHINESE J. OF LASERS, 2003, 30(12), 1075-1078]; [Y X Leng, L H Lin, Z Z Xu, “Spectrum Shaping in a Ti:Sapphire Regenerative Amplifier”, ACTA OPT. SINICA, 2002, 22(02), 170-174]; the CN patent Ser. No. ZL200410025678.1 and the CN patent Ser. No. ZL200410024684.5.

Furthermore, the above literatures also illustrate some defects in the transmission shaping methods, just as following: 1. Using the interference filter for selective transmission, but it exists difficult both in the principle of design and in the fabrication techniques, such as the principle of design can not avoid the Fabry-Perot (FP) side effect. When the modulation bandwidth is less than tens nanometers, the fabrication techniques can not control the bandwidth and the depth in the centre wavelength of the transmittance curve according to the limit of the coating techniques. At the same time, the incident angle of laser is required at high precision and less flexibility. 2. Using the combination lens of birefringent crystal for the selective transmission, here the interference between the ordinary light and the extraordinary light conducts the selective transmission, but it exists difficulty both in the principle of design and in the fabrication techniques. For example, the transmitted element can not avoid the side effect such as FP effect and the distortion of phase etc. Furthermore, the thickness of the birefringent crystal is determined by the spectrum bandwidth of the original pulse, which the law is: the less the bandwidth is, the more the thickness of the birefringent crystal required is. For instance, if the spectrum bandwidth of the ultra-short pulse is 13 nm, the thickness of the birefringent crystal must be 25 mm; however, the size of birefringent crystal can not be produced that large. 3. Using the hinged organic polymer waveguide or using the hinged organic polymer waveguide after a corona poling process for obtaining the characteristics of photoelectric effect for the selective reflection, but it has lower sufferance of the high power laser damages.

SUMMARY OF THE INVENTION

The present invention seeks to provide an improved pulse shaping device to overcome the defects in the traditional shaping devices mentioned above. The new self-collimator concave spectral shaping device for chirped pulse amplification is proposed based on an improved Czerny-Turner Spectrum Instrument (CTSI) system, which involves two symmetrical CTSI systems, called a spectrum decomposing system and a spectrum synthesizing system respectively, and it involves a concave spectrum shaping system. The process is as following: firstly, the chirped pulse is spread totally the frequency components of chirped pulse into a spatial place by the spectrum decomposing system. Then, its spectrum is modulated and shaped by the modulation system in the focus plane. And then, the spatial light is integrated un-shiftily by the spectrum synthesizing system back to a designed shape chirped pulse, which accomplishes the spectrum modulating and shaping function. The present invention has solved the problem that the traditional shaping devices in the world are not applicable for a over terawatt (10¹²) system, or are unusable for a Nd:glass system narrow bandwidth system. The present invention can be not only utilized for a general laser spectrum shaping and spectrum modulating, but also especially utilized for a high energy and ultra-high peak-power laser systems with a few nanometers bandwidth and a large caliber in CPA system. This device has the feature of compacting the structure, requiring less space, and running stability, for its small size of concave reflector, and its self-collimation and its symmetrical distribution. The functional reflector can be manufactured in a large diameter and can be designed on a high damage threshold, so the present invention device can be inserted anywhere in the amplifier chain in the CPA system for extracting large energy and reducing the pedestal of the output. The spectrum modulation ratio can be varied over 60% under the condition that the phase of the reflecting light remains nearly constant. The chromatic resolving capability is about 0.1 nm and the phase aberration in the range of the tens of nanometer is 12 mrad, which could meet the requirement of the kilo joule peta-watt-class reconstruction project.

In order to realize this invention, we have utilized a series of technological schemes as following steps:

A self-collimator concave spectral shaping device for chirped pulse amplification (CPA): the features are the comprising: in the optical path order, the first beam splitter prism, the second beam splitter prism, and the ¼ wave plate; and, the first concave reflector, the first aperture, and the second concave reflector, which these constitute a illumination system; and, the first aperture, the second concave reflector, the grating, the third concave reflector and the concave reflector for spectrum shaping function design, which these constitute a spectrum decomposing system with CTSI construction for self-collimator concave spectral shaping device. In addition, the concave reflector for spectrum shaping function design constitutes a spectrum shaping system. Furthermore, the concave reflector for spectrum shaping function design, the third concave reflector, the grating, the second concave reflector, and the first aperture, which these constitute a spectrum synthesizing system with CTSI construction for self-collimator concave spectral shaping device. The features are the processing: a laser beam from the front-end system of a CPA system passes through the first beam splitter prism for polarization producing; via the ¼ wave plate and the first concave reflector, then it passes through the first concave reflector, the first aperture, and the second concave reflector, which transfer the laser beam into a parallel light. As mentioned above, it passes through the spectrum decomposing system, the spectrum shaping system and the spectrum synthesizing system for self-collimator concave spectral shaping device, which accomplish the spectrum decomposing, the spectrum shaping, and the spectrum synthesizing of the chirped pulse. Then it passes through the ¼ wave plate, its polarization rotates 90 degree, then it is reflected fully by the first beam splitter prism to the second beam splitter prism for a polarization producing of the modulated chirped pulse, and sent into the following stage such as the solid-state amplifier for amplification.

The technological design of the self-collimator concave spectral shaping device, of which the features are: wherein the grating is the reflective planar blazed grating.

The technological design of the self-collimator concave spectral shaping device, of which the features are: wherein all the concave reflectors are made with the chromatic aberration, the spherical aberration, the comatic aberration, the astigmatism and the field curvature eliminated strictly in the whole working frequency bandwidth, to ensure the maximal deviation between the spectrum image curved surface and the surface of the concave reflector for spectrum shaping function design less than the tolerance of the half focal depth.

The technological design of the self-collimator concave spectral shaping device, of which the features are: as the beam reflected by the concave reflector for spectrum shaping function design, its backward wave passing along the inversion optical path, so making the concave spectral shaping device constructed as the self-collimator system.

The technological design of the self-collimator concave spectral shaping device, of which the features are: wherein all the concave reflectors are constructed a symmetrical imaging system relative to the dispersion component, or are constructed an asymmetrical imaging system relative to the dispersion component for compensating the aberration of the image.

The technological design of the self-collimator concave spectral shaping device: the features are that: the first aperture is the aperture diaphragm in the real confocal telescope, which constructed as an illumination system and as an image transfer system. The features are that: the illumination system ensures that the normal width is suitable for the coherence and phase consisted conditions for a incident light, the distribution of a laser beam obtained from the front-end system of a CPA system do not changed in the spatial and temporal domain, the relative aperture in the illumination system must match with the relative apertures in the dispersion system and in the imaging system, and the clear aperture can fill the caliber of the dispersion element. The features are that: the first aperture is the aperture diaphragm in the real confocal telescope, which must meet the normal width a₀ condition for a diaphragm, or the diffraction half width a₀ condition for the spectrum decomposing system and the spectrum synthesizing system, and which can pass through the light with all the frequency components within the chirped laser pulse bandwidth.

The technological design of the self-collimator concave spectral shaping device, of which the features are: wherein the concave reflector for spectrum shaping function design is coated with high reflective and low reflective alternately multilayer dielectric thin films and with micro-structures in it, or a concave reflector for spectrum shaping with micro-mirrors structures in it, or a concave liquid crystal light reflector, or a concave reflector for spectrum shaping with a varied line space grating in front of it, or a concave reflector for spectrum shaping with a liquid crystal spatial light modulator in front of it, or a concave reflector for spectrum shaping with micro-electromechanical mirrors, or a continuous deformation concave reflector for spectrum shaping, or a bimorph deformation concave reflector for spectrum shaping, or a concave reflector for spectrum shaping with a prism/waveguide coupling, or a concave reflector for spectrum shaping with a varied line space grating.

The technological design of the self-collimator concave spectral shaping device, of which the features are: wherein the first beam splitter prism is fully perpendicular to the second beam splitter prism.

The technological design of the self-collimator concave spectral shaping device, of which the features are: wherein all the concave reflectors in the spectrum decomposing system and all the concave reflectors in the spectrum synthesizing system are constructed as a reflective-type horizontal imaging system relative to the dispersion component for the spectroscope, or are constructed as a reflective-type vertical imaging system relative to the dispersion component for the spectroscope.

The technological design of the self-collimator concave spectral shaping device, of which the features are: wherein the spectrum decomposing system and the spectrum synthesizing system are constructed as a reflective-type horizontal shaping system relative to the concave reflector for spectrum shaping function design for the spectroscope, or are constructed as a reflective-type vertical shaping system relative to the concave reflector for spectrum shaping function design for the spectroscope.

The principle of the present invention of the self-collimator concave spectral shaping device for chirped-pulse-amplification (CPA) is that: for a laser spectrum distribution, the device utilizes a symmetrical CTSI spectral decomposition system to decompose truthfully the chirped pulse spectrum to a spatial space, and utilizes a special modulation system to shape the space distribution on the focal plane, and then utilizes a symmetrical CTSI spectral synthesis system to compose un-shiftily this space distribution to a shaped frequency chirped pulse before incidence into the next amplifier stage, which accomplish the chirped pulse spectrum modulation and shaping functions. The present invention is based on selecting the improved CTSI system, and selecting a microstructure on a multilayer dielectric thin film in a concave reflector as a functional reflector to modulate and shape the spectrum of chirped pulse in CPA. Because of adopting an improved CTSI spectral decomposing system and an improved CTSI spectral synthesizing system, the device have more tuning flexibility of the spectrum shaping and modulation. Furthermore, selecting the reflective planar blazed grating can endure the high power laser damage and can be fabricated in a large caliber. And, selecting the concave reflectors are suitable for this rational construction in the collimation system and the imaging system, and are made in strictly corrected the spherical aberration and the comatic aberration, to ensure the maximal deviation between the spectrum image curved surface and the surface of reflector for spectrum shaping function design less than the tolerance of the half focal depth according to the Rayleigh's Criterion. In addition, selecting the rational construction can adjust the position of the dispersion component relative to the two concave reflectors as objective reflectors, in order to minimize the astigmatism and the comatic aberration. The present invention is based on a dispersion system to decompose the chirped pulse spectrum to a spatial space, and a microstructure on a multilayer dielectric thin film as a functional reflector to shape the space distribution, which can shape the spectrum distribution of pre-amplification pulse making it depression in the vicinity of center wavelength in shapes and depths. The details illustrates in the literatures as the CN patent Ser. No. ZL200710049516.5 and the CN patent Ser. No. ZL200720080292.X.

The present invention of device is a self-collimator concave spectral shaping device for chirped-pulse-amplification (CPA), which all optical components are selected as reflective element. The reason is that: a). the device is for a large caliber and high power chirped pulse amplification in huge energy, only the reflective element is suitable, which can endure the high power laser damage and can be fabricated in a large caliber; b). the chromatic aberration can be eliminated in the reflective element easily, and the additional spectrum shaping has the benefit of free, and the spectrum image planar can be straighten in the grating-style spectrum shaping device; c). the reflective element can be worked on almost all the bandwidth of laser, and be utilized in the infrared and the near infrared laser system, especially there is no suitable optical material for fabrication lens in the far infrared and in the far ultraviolet bandwidth. The present invention of device is a self-collimator concave spectral shaping device for chirped pulse amplification (CPA), which all optical components are constructed as symmetrically relative to the dispersion element. The reason is that: a). this kind of construction can cancel the cosmetic aberration to zero; b). this construction relative to the dispersion element symmetrical make compensating the dispersion to zero easily. Furthermore, because of the laser spectrum decomposing and synthesizing, the aperture in the real confocal telescope system substitutes the slit diaphragm in general CTSI system for enhancing light gathering power in the self-collimator concave spectral shaping device.

In CPA practical, to compensate the gain narrowing and the gain saturation, to obtain the shortest compressed pulse, and to improve the SNR of output, people need a kind of spectrum modulation device to shape the spectrum distribution of pre-amplification pulse making it depression in the vicinity of center wavelength in shapes and depths. In the detailed description of the embodiment, the device utilizes a multilayer dielectric thin film in a concave reflector with specific construction to realize the spectrum reshaping of the chirped pulse laser in large energy and high power Nd:glass CPA System. If the parameters of the thin film reflector are chosen differently, the results show that the reflectivity distribution of the multilayer dielectric film reflector can be controlled effectively different on the reflectivity curve and on the relative phase, so as to compensate the gain narrowing and the gain saturation effects.

The beneficial effects of the present invention compared with the traditional technological schemes of spectrum shaping are:

1. The present spectrum shaping device utilizes the improved CTSI system and the concave functional reflector for spectrum shaping design, which decomposes the chirped pulse spectrum, modulates it in the focus plane, then synthesizes the shaped pulse, which has solved the problems that the traditional shaping devices in the world are not applicable to a over terawatt (10¹²) system, or are unusable for a Nd:glass system narrow bandwidth system.

2. The present spectrum shaping device adopts the reflective planar blazed grating, which can endure the high power laser damage and can be fabricated in a large caliber, which has solved the problem that the AOPDF to compensate the spectral gain narrowing gets success just on the structure of a hundred terawatt-class ultra-short laser system such as Ti:sapphire system but not on the Nd:glass system.

3. The present spectrum shaping device is selecting the improved CTSI system, selecting the multilayer dielectric thin film in a concave reflector as a functional reflector for spectrum shaping design with micro-structures in it, and selecting the device of spectrum decomposing, shaping, and synthesizing for CPA, which has solved the problem that a spectrum shaping device do not suitable for a high energy and ultra-high peak-power laser system in the CPA chain with a large caliber and a chirped pulse bandwidth of a few nanometer condition. The present spectrum shaping device is constructed as a self-collimation, which makes the cosmetic aberration and the astigmatic aberration to minimum scale in the centre of the spectrum image, and cancels the aberration in the boundary of the spectrum image to an idea level. Furthermore, the concave reflector is selected as the collimation objective lens or the spectrographic lens, which the chromatic aberration can be made free, and the spectrum image planar can be straighten in the grating-style spectrum shaping device.

4. The present spectrum shaping device has the benefit that it is not only suitable for Ti:sapphire system but also suitable for the Nd:glass system; and has the benefit that the spectrum modulation range can be changed through rotating the reflective planar blazed grating by the axial direction paralleling to the grating groove axis.

5. The present invention of device adopts the reflective planar blazed grating, its modulated light is reflected by the concave reflector for spectrum shaping function design, and the backward wave passes along the inversion optical path, which is constructed as the self-collimation. Therefore this device is featured by less optical components, simple the construction, and easy regulation.

6. The present invention of device is characteristic of small size of concave reflector, easy fabrication, compact construction, little laboratory space needed, and cheap in cost, which has solved the problem that the traditional shaping devices in the world are very complex construction required, or are very expensive for advanced system of chirped pulse shaping.

7. The present spectrum shaping device is selecting the multilayer dielectric thin film as a functional reflector for spectrum shaping design with micro-structures in it, at same time selecting the reflective planar blazed grating, which can endure the high power laser damage and can be fabricated in a large caliber. These measures have solved the problem of the intensity modulation in the reflective large caliber of beam, and which have solved the problem of working under the high pick power condition. So the present invention device can be inserted anywhere in the amplifier chain of CPA system for extracting large energy and reducing the pedestal of the output.

8. The present spectrum shaping device adopts the multilayer dielectric thin film as a functional reflector for spectrum shaping design with micro-structures in it, which has solved the problem that the reflective phase must meet the coherence and the phase consisted condition in the CAP, and which has the benefit that the spectrum modulation ratio can be varied over 60% under the condition that the phase of the reflecting light remains nearly constant.

9. The present spectrum shaping device has the benefit that it can be not only utilized in the ICF spectrum shaping that make the solid-state laser driver ejecting a high-energy in addition to a high peak irradiance, but also can be utilized for a general laser spectrum shaping and spectrum modulation, especially suitable for a high energy and ultra-high peak-power laser system in CPA with a large caliber and a chirped pulse bandwidth of a few nanometers.

10. The present spectrum shaping device adopts the real confocal telescope system, which constructed as an illumination system and as an image transfer construction; which has the benefit that the normal width is suitable for the coherence and the phase consisted conditions; which has solved the problem that the distribution of a laser do not changed in the spatial and temporal domain that the laser beam obtained from the front-end system of a CPA system; which has the benefit that it has a strong light gathering power; which has the benefit that the relative aperture in the illumination system matches with the relative apertures in the dispersion system and in the imaging system; and which has solved the problem that the clear aperture can fill the caliber of the dispersion element.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 schematically illustrates the structure of a self-collimator concave spectral shaping device embodying the present invention

FIG. 2 schematically illustrates the horizontal spatial arrangement shown in the front view of a self-collimator concave spectral shaping device embodying in the example 1 showed in FIG. 1.

FIG. 3 schematically illustrates the vertical spatial arrangement construction shown in the side view of a self-collimator concave spectral shaping device.

FIG. 4 schematically illustrates the vertical spatial arrangement shown in the front view of a self-collimator concave spectral shaping device embodying in the example 2 showed in FIG. 1.

FIG. 5 schematically illustrates the vertical spatial arrangement shown in the front view of a self-collimator concave spectral shaping device embodying in the example 3 showed in FIG. 1.

FIG. 6 schematically illustrates the vertical spatial arrangement shown in the front view of a self-collimator concave spectral shaping device embodying in the example 4 showed in FIG. 1.

FIG. 7 schematically illustrates the vertical spatial arrangement shown in the front view of a self-collimator concave spectral shaping device embodying in the example 5 showed in FIG. 1.

FIG. 8 is a graph schematically illustrating the distribution of spectrum after modulation by the concave functional reflector for spectrum shaping design

FIG. 9 is a graph schematically illustrating the shaped pulse waveform of spectrum after modulation by the present invention as the self-collimator concave spectral shaping device.

In which, 0—the front-end system of CPA; 1—the first concave reflector; 6—the first aperture; 2—the second concave reflector; 3—the grating; 4—the third concave reflector; 5′—the concave reflector for spectrum shaping function design; 7—¼ wave plate; 8—the first beam splitter prism; 9—the second beam splitter prism; 0′—the following amplification stage such as the solid-state amplifier.

DETAILED DESCRIPTION OF THE INVENTION

The following will illustrate the present invention through discussing the working principle and the embodiment with the drawings; however, it should be interpreted as an example of the present invention but not as the definition of the scope of protection of the present invention.

The principle of the self-collimator concave spectral shaping device of the present invention is:

1. The Spectrum Decomposing System

1.1. The Illumination System

The illumination system is used for gathering the light as more energy as possible from the light source, and for transferring the light to the collimation system. In the present invention, the illumination system is composed of a real confocal telescope system including the first concave reflector 1 and the second concave reflector 2; which ensures that the normal width is suitable for the coherence and the phase consisted conditions, and making the distribution of a laser do not changed in the spatial and temporal domain that the seed pulse obtained from the front-end system 0 of a CPA system; which has a strong light gathering power; and which the relative aperture in the illumination system must match with the relative apertures in the dispersion system and in the imaging system, and the clear aperture can fill the caliber of the dispersion element.

1.2. The Collimation System

Because the grating should working on the parallel light in the spectrum decomposing system and in the synthesizing system, the illumination light needs to be changed by a collimation system, which utilizes concave reflectors to fulfill the collimation function. In the optical path order, a light from the incident aperture such as the first aperture 6 in this system construction is changed by the second concave reflector 2 into a parallel light, and then it illuminates the grating 3; called the illumination system. Usually the illumination system is composed of a slot and an objective lens, where the slot is posited in the front focus of the objective lens. However, the aperture in present invention is the aperture diaphragm in the real confocal telescope under the cause of a laser illumination, which replaces the slot in the illumination system, which is the real light source for the following system, and which is the boundary of the beam of an incident light.

1.3. The Dispersion System

The dispersion system is used for decomposing the spectrum of the compound light to a spatial space. However, the spectroscopic prism has a lower dispersive power, and the image of spectrum of the prism inherently has a tilt and distortion, so the spectrum prism is not applicable to the CPA spectrum shaping system. The multiple-beam interferometer such as Fabry-Perot and Lu Mu-mageik parallel plate has a high-resolution of dispersion, but it can not blaze and it can not endure the high laser energy, and its optical path can not be reversible, so the multiple-beam interferometer is not selected. The concave grating system is simple in construction, but its fabrication can not be easy, its effective area is small, its image can not be clear, its astigmatism is large, and its linear dispersion can not be uniform, so the concave grating is not selected. The spectrum filter is a transmission element, which it has lower sufferance of the high power laser damages, and the transmitted element can not avoid the side effect such as FP effect and the distortion of phrase etc., so the spectrum filter is not selected. The echelon grating has a high-resolution of dispersion, but it can not be fabricated easily, and its free spectral range is very small, so the echelon grating is not selected. Therefore, the reflective planar blazed grating is selected in the present invention, which can endure the high energy and high power laser damage, and which can be fabricated in a large caliber.

1.3.1 The Principle of Spectrum Grating Decomposing

As a light incidents and diffracts in the principal section of grating, the maximum condition of interference of two adjacent rays defines the grating equation as

d ₁(sin α₁+sin β₁)=m ₁λ  (1)

where α₁ is the incident angle relative to the spectrum decomposing grating β₁ is the diffraction angle relative to the spectrum decomposing grating; d₁ is the grating space relative to the spectrum decomposing grating, called the grating constant; m₁ is the order of spectrum relative to the spectrum decomposing grating that is an integer; λ is the wavelength. Then Eq. (1) changes to

$\begin{matrix} {{\beta_{1}(\lambda)} = {\arcsin \left( {\frac{m_{1}\lambda}{d_{1}} - {\sin \; \alpha_{1}}} \right)}} & (2) \end{matrix}$

Apparently, the Eq. (2) illustrates that: when the grating space d₁ and the incident angle α₁ is given, the diffraction angle β₁ is larger correspond to the wavelength λ longer in the same order of spectrum of the grating m₁ level except the zero level. Therefore, the great light of different wavelengths at the same level of the main value appears in the same location of different spaces, which spreads the spectrum by the order from the short wavelength to the long wavelength, from zero level to the larger level of the main value, locating beside the zero level at right and left. Typically, the diffraction angle for a long wavelength is larger than that for a short one, and the distribution of diffractive light is strictly linear, coinciding with the order of wavelength. Because the number of grating grooves is huge, the angular breadth of the great light of diffraction light is mince, which its effect is alike that the fringe is sharper in the fringes pattern. So the pattern of the grating diffraction after the objective lens is a fine and bright line in the focus plane—the spectrum line in practice.

1.3.2 The Principle of Spectrum Grating Synthesizing

Described in the geometrical optics: the great light of different wavelengths at the same level of the main value appears in the same location of different spaces, which the distribution of diffractive light is strictly linear, coinciding with the order of wavelength. Inversely, when the monochromatic light incident in the diffraction angle β(λ) coinciding with the order of wavelength is converged onto a grating, the grating can combine these monochromatic lights in the order of wavelength to a synthesizing light in the space, which is the result of the multiple-slit diffraction and interference in principle. The great light of the synthesizing light from the grating is determined by the primary maximum conditions for the grating diffraction pattern of all different monochromatic lights. Usually the reflective planar blazed grating is utilized as the spectrum synthesizing element. Therefore, as light incident into a main surface, the maximum condition of interference of two adjacent rays defines the grating equation as:

d ₂(sin α₂+sin β₂)=m ₂λ  (3)

which, α₂ is the incident angle relative to the spectrum synthesizing grating; β₂ is the diffraction angle relative to the spectrum synthesizing grating; d₂ is the grating space relative to the spectrum synthesizing grating, called grating constant; m₂ is the order of spectrum relative to the spectrum synthesizing grating that is an integer. If the energy loss is neglected, and if all the diffraction lights are a convergent-type spherical wave synthesizing, substituting the Eq. (2) into Eq. (3), that is α₂(λ)=β₁(λ), the grating equation is:

$\begin{matrix} {{d_{2}\left( {{\sin \left( {\arcsin \left( {\frac{m_{1}\lambda}{d_{1}} - {\sin \; \alpha_{1}}} \right)} \right)} + {\sin \; \beta_{2}}} \right)} = {m_{2}\lambda}} & (4) \end{matrix}$

When d₂=d₁, and m₂=m₁, the Eq. (4) changes to

sin β₂=sin α₁  (5)

If the principal range is (0, π/2), from the Eq. (5), we have

β₂=α₁  (6)

The Eqs. (4), (5) and (6) illustrate that: the grating can combine these monochromatic lights in the order of wavelength to a synthesizing light in the space when the output angle β₂(λ) is equal to the incident angle α₁ that is in the spectrum decomposing; when a monochromatic light as a convergent-type spherical wave incident in the diffraction angle

${\beta_{1}(\lambda)} = {\arcsin \left( {\frac{m\; \lambda}{d} - {\sin \; \alpha_{1}}} \right)}$

into the spectrum synthesizing grating; when the grating constants are the same in the spectrum decomposing grating and the spectrum synthesizing grating, which is d₂=d₁; when the order of spectrum of grating are the same in the spectrum decomposing and synthesizing, which is m₂=m₁; and when the grating blazed, which the principal range is (0, π/2). Therefore, the output angle for all the monochromatic lights is equal to a constant, which is the result of the multiple-slit diffraction and interference in principle. In practical, selecting the monochromatic lights in the first level of the grating diffraction pattern that concentrates more than 90% energy for synthesizing, so the great light of the synthesizing light from the grating is bright, and its position is determined by the primary maximum condition for the grating diffraction pattern of all the different monochromatic lights, which is β₂=α₁. Usually the reflective planar blazed grating is utilized as the spectrum synthesizing element.

The following will discuss how to select the geometrical parameters of a synthesizing grating, taking the reflective planar blazed grating with slope surface of gold plating grooves as an example. The geometrical parameters of a reflective planar blazed grating is defined as following: there is a slope surface A of the reflective planar blazed grating with slope surface of gold plating grooves, where b is the width of the grooved surface, t is the angle of the groove mode, and d is the grating constant. According to the requirement of concentrating all the light energy to a certain order of spectrum of grating, the primary maximum of the diffraction light must coincide with the reflective light from the slope surface that is the diffraction light in zero level, where the equation is

$\begin{matrix} {{2\; \sin \mspace{11mu} t\; {\cos \left( {{\alpha_{2}(\lambda)} - t} \right)}} = \frac{m\; \lambda}{d}} & (7) \end{matrix}$

At the same time, the primary maximum of the diffraction light in zero level of the grating spectrum must coincide with the primary minimum of the diffraction light in the first level when the slope surface A is a single slit for diffraction, where b is its width of the grooved surface; hence the equation becomes

$\begin{matrix} {{2\; \sin \mspace{11mu} t\; {\cos \left( {\alpha_{2}(\lambda)} \right)}} = \frac{\lambda}{b}} & (8) \end{matrix}$

When the order of grating of spectrum, the wavelength and the incident angle are defined by the Eqs. (1)-(6), the fabrication section parameters (b, d, t) can be calculated from the Eqs. (7) and (8). So the general condition of a planar blazed grating, called the Vice Blazed Condition, should be

$\begin{matrix} {t = \frac{\alpha_{2} + \beta_{2}}{2}} & (9) \end{matrix}$

which, t is the angle of the Groove Mode that is the angle between the grooved surface and the plane of grating or the angle between the normal line n of the grooved surface and the normal line n of the plane of grating, called the grating blazed angle. When the grating works under the Littrow mounting, which is α₂=β₂=t, called the primary diffraction condition, we have:

$\begin{matrix} {{{\sin \; 2t} = \frac{\lambda_{B}}{b}},{{2\; \sin \mspace{11mu} t} = \frac{\lambda_{B}}{d}}} & (10) \end{matrix}$

Usually the grating is working under the wavelength range

${\frac{\lambda}{d} < 0.8},$

and using its first diffraction level in the self-collimation construction, in order to get the highest diffraction efficiency and the largest free spectral range. However, the practical grating experiments show that the Grating Wood Abnormality is something related to the polarization of the incident light, although the grating is designed coinciding with the principle of the grating geometric parameters design mentioned above. Therefore we choose the system structure, which is not worked exactly on the self-collimation to avoid the Grating Wood Abnormality. So the blazed direction under the non-Littrow mounting is

θ_(b)=β₂=2t−α ₂(λ)  (11)

and the blazed wavelength under the Vice Blazed Condition is

$\begin{matrix} \begin{matrix} {\lambda_{b} = {\lambda_{B}\; \cos \frac{\delta_{b}}{2}}} \\ {= {\lambda_{B}{\cos \left( \frac{\beta_{2} - \alpha_{2}}{2} \right)}}} \\ {= {\lambda_{B}{\cos \left( {t - {\arcsin \left( {\frac{m_{1}\lambda}{d_{1}} - {\sin \; \alpha_{1}}} \right)}} \right)}}} \end{matrix} & (12) \end{matrix}$

which, δ_(b) is the angle between the incident light and the diffraction light, λ_(B), λ_(b) are the blazing wavelengths under the blazed direction and the Vice Blazed Condition. The Eqs. (11) and (12) show that: if the centre-wavelength blazing, the peripheral wavelength blazes its output although the diffraction efficiency is a bit lower than that in centre wavelength. Hence, the reflective planar grating blazing for the centre-wavelength is selected for the spectrum synthesizing element, and for the decomposing grating element.

The rigorous wave theory has proved the mechanism of the spectrum grating synthesizing, that is: If the position of a spectrum distribution in the spectral plane is (−f, y_(m)), where −f is the front focus plane of the objective lens where the spectrum distribution before synthesizing is in here; and y_(m) is the position of the monochromatic light in the spectrum vertical distribution; And, the position of the diffraction grating is (f, 0) that is in the back focus; In addition, let the centre-wavelength locates in the optical axis, let the primary maximum of the grating grooves diffraction coincides with the primary maximum of interference of the minus first (−1) level, and let the primary maximum of interference of the zero (0) level coincides with the primary minimum of grating grooves diffraction of the first (+1) level; Furthermore, let the another wavelength locate in the up and down of the optical axis, let the primary maximum of interference of the minus first (−1) level of other wavelength coincides with the primary maximum of grating grooves diffraction of the centre-wavelength; And let the angle between the normal line n of the grating plane and the optical axis of the objective lens be a half of the angle of Groove Mode t, where d is about 1 μm; Therefore, the diffraction output of the compound light obtains the characteristics that the beams overlap each other in the near-field and the far-field well, the half-angular width of the output beam is mince, the intensity of the output is strong, the diffraction efficiency is large, and the energy utilization of the incident light is more effective. Further more, using this kind of spectrum grating synthesizing, the beam quality can reach the nearly diffraction limited quality, where the law is that the smaller the angle of groove mode t is, the smaller the half-angular width of the output beam is.

1.4 The Image System

The image system is used for converging the spread diffraction lights in the order of wavelength onto the focus plane of the objective lens, forming an array of monochromatic image in the order of wavelength spectrum. There are three kinds of spectrum patterns for different research objects: the line spectrum, the band spectrum, and the continuous spectrum. As for chirped pulse decomposing, shaping, and synthesizing, the spectrum pattern in the chirped pulse bandwidth is a continuous spectrum or the first level band spectrum.

In addition, the image system is used for compensating the comatic aberration and the astigmatism correction. The spherical aberration in the image system can not be cancelled by adjusting the element position, but it must be corrected to less than the tolerance of the image system aberration and the collimation system aberrations in the fabrication and design stages. When the concave reflector is used just as a collimation lens and an objective lens, selecting the paraboloid reflector can cancel the spherical aberration. However, the comatic aberration can be cancelled by adjusting the collimation lens' and the objective lens' position, and designing a special construction to correct. In the present invention, adjusting the relative position between the dispersion element and two concave reflectors as the objective lens eliminates the comatic aberration. In addition, the astigmatism in the image system can not be cancelled by selecting an appropriate geometrical parameter of the concave reflector in the fabrication when the concave reflector is used as a collimation lens and an objective lens. However, the astigmatism can be cancelled by adjusting the relative position of the dispersion element and the two objective reflectors, and designing a special construction to correct.

2. The Spectrum Shaping System

The spectrum shaping system is composed of a concave reflector for spectrum shaping function design 5′, where the chirped pulse passes through the image system via the concave reflectors projecting onto this functional reflector. The concave reflector for spectrum shaping function design 5′ is a microstructure on a multilayer dielectric thin film in a concave reflector as a functional reflector to shape the space distribution, where the outer part of the pagoda-step microstructure is the high reflective thin film system and the pagoda-step microstructure is the antireflective thin film system. The high reflective thin film system accomplishes the diffraction intensity modulation as chirped pulse passing grating system, while the antireflective coating microstructure increases the flexibility of the spectrum modulation. With the pagoda-step of the microstructure, a different step level of the mirror corresponds to the horizontal location of the spectra modulating, where all reflected light has a same phase, which make a depression. Therefore, the intensity on the surface of the functional reflector is the shaped spectra. The FIG. 8 illustrates that: this concave reflector for spectrum shaping function design can make a depression in the vicinity of the center wavelength to shape the reflective intensity into a designed spectrum distribution, where curve 1 is the incident chirped pulse spectrum, curve 2 is the modulation curve of a multilayer dielectric reflector determined by the microstructure, and curve 3 is the distribution of chirped pulse spectrum after modulation.

In present invention of device, the modulated light is reflected and modulated by the concave reflector for spectrum shaping function design 5′, its backward wave passes along the inversion optical path because the device construction has the feature of the self-collimation. At the same time, the microstructure in the concave reflector for spectrum shaping function design 5′ can make a depression in the vicinity of the center wavelength to shape the reflective intensity into a designed spectrum distribution. Therefore, a suitable pre-amplification pulse, which meets the requirement of the spectrum shaping of a high energy and high power CPA system, can be accomplished by designing the microstructure and controlling the processing accuracy rationally.

3. The Spectrum Synthesizing System

According the principle of spectrum grating synthesizing: the great light of different wavelengths at the same level of the main value appears in a monochromatic distribution of diffractive light linearly, when the monochromatic lights incidences in the diffraction angle β(λ) converging onto a grating, the grating can combine this monochromatic lights in the order of wavelength to a synthesized light in the space. Described in the spectrum synthesizing system optical path order, the modulation light is reflected and modulated by the concave reflector for spectrum shaping function design 5′. The reflected light form the concave functional reflector passes through the collimation lens such as the third concave reflector 4 transformed into a parallel light projecting onto the grating, which accomplished the spectrum imaging, the dispersion cancelling, and the synthesizing functions. Finally it images onto a output aperture ejecting out by a concave imaging reflector such as the second concave reflector 2. At this point, all these above is the whole spectrum synthesizing unit, called the spectrum synthesizing system with CTSI construction.

The spectrum synthesizing system is composed of a symmetrical dispersion system and a symmetrical image system after the concave reflector for spectrum shaping function design 5′, in which the features are that: the spectrum synthesizing system images self-collimating to the spectrum decomposing system, cancels dispersion unanimously to the spectrum decomposing system, and subtracts the optical path difference of the different monochromatic lights to zero, which make the extra residual dispersion be zero practically. The construction of the present invention of device is a self-collimation optical path construction, because the spectrum synthesizing system with the CTSI structure is formed from the reflection by the concave reflector for spectrum shaping function design 5′, which is symmetrically to the spectrum decomposing system with the CTSI structure.

Therefore, we must design the spectrum decomposing system with the CTSI construction and the spectrum synthesizing system with the CTSI construction exactly the same and the symmetrical, in which the focal length of the collimation system and the focal length of the imaging system are equal, and also the lateral magnification are equal; or in which the construction of the spectrum decomposing system and the spectrum synthesizing system are absolutely symmetrical; furthermore, in which tracing in the inversion optical path direction, the focal length of a collimation system and the focal length of a imaging system are equal, and also the lateral magnification are equal. Hence, the extra residual dispersion can be made to zero practically under the condition that the widths of all apertures and their images are equal.

5. The Tolerance of the Image and Collimation System Aberrations

Before assembling the spectrum shaping system, the spectrum decomposing system with CTSI construction and the spectrum synthesizing system with CTSI construction must firstly correct the aberration respectively, which ensures that the total aberration must be within the tolerance of engineering aberration design. The requirement of the aberration correction can be summarized by: 1. making the spectrum image plane straight in the whole visual field; 2. making the spectrum clear and symmetrical in the whole spectrum plane; 3. making the intensity distribution of the spectrum uniform along the vertical direction. Furthermore, because the collimation system of the spectrum decomposing system with CTSI construction and the spectrum synthesizing system with CTSI construction is characterized by a small relative aperture and a small visual field, the imaging system of this system is also a small relative aperture and a middle visual field system.

In addition, the requirement for the parameter of aberration correction can be summarized as that all the objective reflectors of the collimation system and the imaging system are made with strictly correcting the spherical aberration and the comatic aberration. Empirically, we select the Rayleigh's Criterion as the tolerance of the imaging and collimation system's aberrations, where the Rayleigh's Criterion is that the maximum wave aberration of the residual spherical aberration and the residual comatic aberration must be less than λ/4. According to the relation between the wave aberration and the axial aberration, the tolerances of the spherical aberration and the comatic aberration of the concave reflectors are the axial spherical aberration:

$\begin{matrix} {{LA}^{\prime} \leq {\frac{8}{3}{\lambda \left( \frac{f^{\prime}}{D} \right)}}} & (13) \end{matrix}$

the deflection sine condition

$\begin{matrix} {{OSC}^{\prime} \leq {\frac{\lambda}{nl}\left( \frac{f^{\prime}}{D} \right)}} & (14) \end{matrix}$

where, D is the diameter of the effective aperture, which is the effective size of the dispersion element in the spectrum decomposing system with CTSI construction and the spectrum synthesizing system with CTSI construction; f′ is the focal length of the objective lens; λ is the wavelength of a certain light; l is the distance between the principal ray in the boundary or the spectrum in the boundary and that in the optical axis.

At the present invention, selecting the concave reflector as the collimation objective lens and as the imaging objective lens in all structure, the spherical aberration can not be cancelled by adjusting the elements position. And when the spherical aberration needs to be corrected especially, the concave reflector can be substituted by an aspherical reflector. However, because the primary comatic aberration of the parabolic reflector is larger than that of the spherical reflector, the spherical reflector is used universally. Therefore, if the system must adopt the spherical reflector, the size of the relative aperture must be controlled to make the diameter of the disc of confusion of the spherical aberration less than the tolerance of the normal width a₀.

Furthermore, the comatic aberration can be cancelled by adjusting the relative positions of the two objective reflector's positions. Hence considering the two objective reflectors together, the present invention selects designing an improved CTSI special construction and controls the size of the relative aperture to correct the comatic aberration to near zero.

Straightening the spectrum plane: the maximal deviation between the spectrum image surface and the surface of the concave reflector for spectrum shaping function design must be less than the tolerance of the half focal depth, which is

$\begin{matrix} {{\frac{1}{2}\Delta \; F} \leq {2{\lambda \left( \frac{f^{\prime}}{D} \right)}^{2}}} & (15) \end{matrix}$

where, ΔF is the focal depth. Usually the bending of the spectrum plane is dominated by the chromatic aberration of the collimation system and the imaging system, and straightening the spectrum plane is resulted from the compensation between the chromatic aberration and the field curvature in the meridian plane of the collimation and the image objective reflectors. However, in present invention, because the lateral magnification of the grating changes slightly with the wavelength difference, so the method mention above can not be adopted. Therefore, all the objective lenses should be made with strictly eliminating the chromatic aberration, hence selecting the concave reflector as the collimation and imaging objective lens in the present invention.

6. The Configuration of the Device

All the concave reflectors, the dispersion components, and the aperture in the spectrum decomposing system and those in the spectrum synthesizing system, and all their images are in a horizontal planar, called constructed as a reflective-type horizontal imaging construction for the spectroscope system. However, all the concave reflectors, the dispersion components, and the aperture in the spectrum decomposing system and those in the spectrum synthesizing system, and all their images are in a vertical planar, called constructed as a reflective-type vertical imaging construction for the spectroscope system. Furthermore, the spectrum synthesizing system is horizontally symmetrical to the spectrum decomposing system relative to the dispersion component, defined as a reflective-type horizontal imaging spectrum shaping system. However, the spectrum synthesizing system is vertically symmetrical to the spectrum decomposing system relative to the dispersion component, defined as a reflective-type vertical imaging spectrum shaping system. Because the functional reflector for spectrum shaping design could make a parasitic diffraction in the horizontal direction, but it is just a planar reflector in the vertical direction, so we select the construction as a reflective-type vertical imaging construction for the spectroscope system in present invention. However, when the width of step of the microstructure in the functional reflector for spectrum shaping design is tens times the wavelength, the parasitic diffraction in the horizontal direction of the functional reflector for spectrum shaping design is too little to be observed. At this time, the construction as a reflective-type horizontal imaging spectrum shaping system can be utilized. The circumstance, where the device settled and which the imaging quality of the physical experiments required, dominates what construction can be selected.

DETAILED DESCRIPTION OF THE EMBODIMENT Example 1 of the Device

In this example 1, there are those: the grating 3 is the reflective planar blazed grating, which can endure the high power laser damage and can be fabricated in a large caliber. The concave reflector for spectrum shaping function design 5′ is a concave reflector coated a multilayer dielectric thin film with microstructures in it as a concave functional reflector for spectrum shaping. All the concave reflectors are made in strictly eliminated the chromatic aberration, the spherical aberration, and the comatic aberration, to ensure the maximal deviation between the spectrum image curved surface and the surface of the concave reflector for spectrum shaping function design less than the tolerance of the half focal depth deduced from the Rayleigh's Criterion. The first aperture 6 is an aperture diaphragm, also is the incident aperture, and the output aperture.

FIG. 1 schematically illustrates the structure of a self-collimator concave spectral shaping device embodying the present invention, which the above elements are settled in this optical path construction. In present invent of device, the spatial arrangement of a self-collimator concave spectral shaping device is: all the concave reflectors, the dispersion components, and the aperture in the spectrum decomposing system and those in the spectrum synthesizing system formed after the concave reflector for spectrum shaping function design 5′, and all their images are in a horizontal planar. That is to say, this spatial arrangement of self-collimator concave spectral shaping device is constructed as a reflective-type horizontal imaging construction for the spectroscope system showed in FIG. 2. The parameters of the design requirement, the spatial arrangement, and the optical element showed in table 1, which are:

TABLE 1 the parameters of the design requirement, the spatial arrangement, and the optical element Item Parameters Diameter of the incidence Normal width 105.3 μm Resolution of line dispersion 0.1 nm/mm Distance between 3000 mm the collimation lens and the imaging lens Value of relative aperture 1:100 Distance between the grating and 2550 mm the collimation lens or the objective lens Incident angle of the grating 66.36385°     as the Littrow angle Diameter of 30 mm the incident light onto the grating Density of the grating groove 1740 g/mm Fluence of the grating working 0.5 J/cm{circumflex over ( )}2 Size of the reversible grating 3 100 mm × 50 mm × 20 mm Size of the first concave reflector 1 30 mm × 40 mm, R0.6 m* Size of the second concave reflector 2 292 mm × 40 mm, R6 m* Size of the third concave reflector 4 292 mm × 40 mm, R6 m* Size of the centro-symmetric concave reflector 4″ 292 mm × 40 mm, R6 m* Size of the concave reflector for 440 mm × 100 mm × 40 mm R6 m* spectrum shaping function design 5′ Bandwidth of the non-apodized spectra of 24 nm the concave reflector for spectrum shaping function design 5′ Diameter of the first aperture 6 270.89 μm Angle ∠012 between the axis and the centre line of 8° the first concave reflector 1 off-axis settled Angle ∠123 between the axis and the centre line of 8° the second concave reflector 2 off-axis settled Angle ∠234 between the incident light and 132.7277°     the diffraction light on the reversion grating 3 Angle ∠345′ between the axis and the centre line of 8.7335°    the third concave reflector 4 off-axis settled Angle ∠45′4 between the axis and the centre line of 0° the concave functional reflector 5′ off-axis settled Note: *(radius of curvature)

The self-collimator concave spectral shaping device decomposing system: describing in the optical path order, a laser beam from the front-end system of a CPA system passes through the first beam splitter prism 8 for polarization producing, then it passes through the ¼ wave plate 7 as the p-polarized light in Brewster's angle incidence. And then it passes through the first concave reflector 1 and the second concave reflector 2, which constitute the image transfer construction. Then it focuses onto the first aperture 6. Hence the illumination system is composed of the first concave reflector 1, the first aperture 6, and the second concave reflector 2. Here the first aperture becomes the incident aperture of the spectrum shaping structure in example 1. Then the laser beam passes through the second concave reflector 2, where it is transformed into a parallel light, and then it is projected onto the grating 3, which constitutes the collimation system. However, because of the laser illumination, the first aperture 6 substitutes the slit diaphragm in general CTSI system, and serves as the real light source for the following system, which is the boundary of the beam of an incident light entering into the structure of self-collimator concave spectral shaping device. The laser beam from the first aperture 6 passes through the second concave reflector 2, where it is transformed into a parallel light, and then it is projected onto the grating 3, which comprises the dispersion system. After that, the diffraction light passes through the third concave reflector 4 imaging onto the concave reflector for spectrum shaping function design 5′. All these above constitute the whole spectrum decomposing system, which is denoted by the optical path order 6-2-3-4-5′.

The spectrum shaping system of the self-collimator concave spectral shaping device: The concave reflector for spectrum shaping function design 5′ is a concave reflector coated a multilayer dielectric thin film consisting of alternately arranged high reflective and low reflective material with micro-structures in it as a concave functional reflector for spectrum shaping, which makes the spectrum of chirped pulse a depression in the vicinity of the center but keeps the phase of the reflecting light nearly constant. Furthermore, the spectrum shaping system requires that the maximal deviation between the spectrum image surface and the surface of the concave reflector for spectrum shaping function design 5′ is less than the tolerance of the half focal depth, which is deduced from the Rayleigh's Criterion, and requires that the diameter 2 dr′ of the disc of confusion in the focus plane, or the width a′ of the disc of confusion in the direction of the dispersion are less than a certain value a₀ in the surface of the concave reflector for spectrum shaping function design 5′. The FIG. 8 illustrates that: this the concave reflector for spectrum shaping function design 5′ can make a depression in the vicinity of the spectral center to shape the reflective intensity into a designed spectrum distribution, where curve 1 is the incident chirped pulse spectrum, curve 2 is the modulation curve of a multilayer dielectric reflector determined by the microstructure, and curve 3 is the distribution of chirped pulse spectrum after modulation.

The self-collimator concave spectral shaping device synthesizing system: the diffraction light from the concave reflector for spectrum shaping function design 5′ reflected by itself passes along the inversion optical path. So this construction in example 1 is the same as the self-collimation imaging system and the self-collimation dispersion system. The features of the self-collimator concave spectral shaping device synthesizing system are that the structure in optical path in this example 1 is simple, compact and different from the Littrow system. When the backward wave passes through the above CTSI decomposing system 6-2-3-4-5′, this structure in the inversion optical path constitutes the self-collimation CTSI spectrum synthesizing system, which accomplishes the dispersion cancelling function. Described by the inversion optical path, the modulation light from the concave reflector for spectrum shaping function design 5′ passes through the third concave reflector 4, where it is collimated onto the grating 3, which these comprise a dispersion cancelling construction; then, the parallel light from the grating incident into the second concave reflector 2 focused onto the first aperture 6, which constitute a spectrum synthesizing system with the CTSI construction. All these above constitute the whole spectrum synthesizing system, which is noted by the optical path order 5′-4-3-2-6. Via the first concave reflector 1, it is transferred into a parallel light and accomplished the spectrum decomposing, shaping, and synthesizing. And via the ¼ wave plate 7, its polarization rotates 90 degree; then it is reflected fully at the first beam splitter prism 8 to the second beam splitter prism 9 that is perpendicular to the first one for cancelling the stray light of the modulated chirping pulse, then it is sent into the following stage 0′ such as the solid-state amplifier to be amplified. In present invention of device, the modulated light is reflected and modulated by the concave reflector for spectrum shaping function design 5′, its backward wave via the third concave reflector 4 images onto the dispersion system, which this construction features as the self-collimation system. The diffraction light is reflected back along the inversion optical path order and is projected to the dispersion system, making the extra residual dispersion be zero practically. FIG. 9 is a graph schematically illustrating the shaped pulse waveform of spectrum after modulation by the construction in FIGS. 1 and 2. And FIG. 9 illustrates that this self-collimator concave spectral shaping device makes a depression in the centre wavelength of 1053 nm, and the spectrum modulation ratio can be controlled over 60% under the condition that the phase of the reflecting light remains nearly constant.

In the example 1, the a concave reflector for spectrum shaping function design 5′ could be a multilayer dielectric thin film on a concave reflector for spectrum shaping with micro-structures in it, or a concave reflector for spectrum shaping with micro-mirrors structures in it, or a concave liquid crystal light reflector, or a concave reflector for spectrum shaping with a varied line space grating in front of it, or a concave reflector for spectrum shaping with a liquid crystal spatial light modulator in front of it, or a concave reflector for spectrum shaping with micro-electromechanical mirrors, or a continuous deformation concave reflector for spectrum shaping, or a bimorph deformation concave reflector for spectrum shaping, or a concave reflector for spectrum shaping with a prism/waveguide coupling, or a concave reflector for spectrum shaping with a varied line space grating.

Example 2 of the Device

In this example 2, there are those: the grating 3 is the reflective planar blazed grating, which can endure the high power laser damage and can be fabricated in a large caliber. The concave reflector for spectrum shaping function design 5′ is a concave reflector coated a multilayer dielectric thin film with microstructures in it as a concave functional reflector for spectrum shaping. All the concave reflectors are made in strictly eliminated the chromatic aberration, the spherical aberration, and the comatic aberration, to ensure the maximal deviation between the spectrum image curved surface and the surface of the concave reflector for spectrum shaping function design less than the tolerance of the half focal depth deduced from the Rayleigh's Criterion. The first aperture 6 is an aperture diaphragm, also is the incident aperture, and the output aperture.

FIG. 1 schematically illustrates the structure of a self-collimator concave spectral shaping device embodying the present invention, which the above elements are settled in this optical path construction. In present invent of device, the spatial arrangement of a self-collimator concave spectral shaping device is: all the concave reflectors, the dispersion components, and the aperture in the spectrum decomposing system and those in the spectrum synthesizing system formed after the concave reflector for spectrum shaping function design 5′, and all their images are in a vertical planar. That is to say, the spatial arrangement of self-collimator concave spectral shaping device is constructed as a reflective-type vertical imaging construction for the spectroscope system showed in FIGS. 3 and 4. The parameters of the design requirement, the spatial arrangement, and the optical element showed in table 2, which are:

TABLE 2 the parameters of the design requirement, the spatial arrangement, and the optical element Item Parameters Diameter of the incidence Ø3 mm Normal width 105.3 μm Resolution of line dispersion 0.1 nm/mm Distance between 3000 mm the collimation lens and the imaging lens Value of relative aperture 1: 100 Distance between the grating and 2550 mm the collimation lens or the objective lens Incident angle of the grating    66.36385° as the Littrow angle Diameter of Ø30 mm the incident light onto the grating Density of the grating groove 1740 g/mm Fluence of the grating working 0.5 J/cm{circumflex over ( )}2 Size of the reversible grating 3 100 mm × 50 mm × 20 mm Size of the first concave reflector 1 Ø30 mm × 40 mm, R0.6 m* Size of the second concave reflector 2 Ø292 mm × 40 mm, R6 m* Size of the third concave reflector 4 Ø292 mm × 40 mm, R6 m* Size of the centro-symmetric concave reflector 4″ Ø292 mm × 40 mm, R6 m* Size of the concave reflector for 440 mm × 100 mm × 40 mm R6 m* spectrum shaping function design 5′ Bandwidth of the non-apodized spectra of 24 nm the concave reflector for spectrum shaping function design 5′ Diameter of the first aperture 6 270.89 μm Angle ∠012 between the axis and the centre line of 8° the first concave reflector 1 off-axis settled projecting on the horizontal Angle ∠012 between the axis and the centre line of 6° the first concave reflector 1 off-axis settled projecting on the vertical Angle ∠123 between the axis and the centre line of 8° the second concave reflector 2 off-axis settled projecting on the horizontal Angle ∠123 between the axis and the centre line of 6° the second concave reflector 2 off-axis settled projecting on the vertical Angle ∠234 between the incident light and 0° the diffraction light on the reversion grating 3 projecting on the horizontal Angle ∠234 between the incident light and 6° the diffraction light on the reversion grating 3 projecting on the vertical Angle ∠345′ between the axis and the centre line of    8.7335° the third concave reflector 4 off-axis settled projecting on the horizontal Angle ∠345′ between the axis and the centre line of 6° the third concave reflector 4 off-axis settled projecting on the vertical Angle ∠45′4 between the axis and the centre line of 0° the concave functional reflector 5′ off-axis settled Note: *(radius of curvature)

The self-collimator concave spectral shaping device decomposing system: describing in the optical path order, a laser beam from the front-end system of a CPA system passes through the first beam splitter prism 8 for polarization producing, then it passes through the ¼ wave plate 7 as the p-polarized light in Brewster's angle incidence. And then it passes through the first concave reflector 1 and the second concave reflector 2, which constitute the image transfer construction. Then it focuses onto the first aperture 6. Hence the illumination system is composed of the first concave reflector 1, the first aperture 6, and the second concave reflector 2. Here the first aperture becomes the incident aperture of the spectrum shaping structure in example 2. Then the laser beam passes through the second concave reflector 2, where it is transformed into a parallel light, and then it is projected onto the grating 3, which constitutes the collimation system. However, because of the laser illumination, the first aperture 6 substitutes the slit diaphragm in general CTSI system, and serves as the real light source for the following system, which is the boundary of the beam of an incident light entering into the structure of self-collimator concave spectral shaping device. The laser beam from the first aperture 6 passes through the second concave reflector 2, where it is transformed into a parallel light, and then it is projected onto the grating 3, which comprises the dispersion system. After that, the diffraction light passes through the third concave reflector 4 imaging onto the concave reflector for spectrum shaping function design 5′. All these above constitute the whole spectrum decomposing system, which is denoted by the optical path order 6-2-3-4-5′.

The spectrum shaping system of the self-collimator concave spectral shaping device: The concave reflector for spectrum shaping function design 5′ is a concave reflector coated a multilayer dielectric thin film consisting of alternately arranged high reflective and low reflective material with micro-structures in it as a concave functional reflector for spectrum shaping, which makes the spectrum of chirped pulse a depression in the vicinity of the center but keeps the phase of the reflecting light nearly constant. Furthermore, the spectrum shaping system requires that the maximal deviation between the spectrum image surface and the surface of the concave reflector for spectrum shaping function design 5′ is less than the tolerance of the half focal depth, which is deduced from the Rayleigh's Criterion, and requires that the diameter 2 dr′ of the disc of confusion in the focus plane, or the width a′ of the disc of confusion in the direction of the dispersion are less than a certain value a₀ in the surface of the concave reflector for spectrum shaping function design 5′. The FIG. 8 illustrates that: this the concave reflector for spectrum shaping function design 5′ can make a depression in the vicinity of the spectral center to shape the reflective intensity into a designed spectrum distribution, where curve 1 is the incident chirped pulse spectrum, curve 2 is the modulation curve of a multilayer dielectric reflector determined by the microstructure, and curve 3 is the distribution of chirped pulse spectrum after modulation.

The self-collimator concave spectral shaping device synthesizing system: the diffraction light from the concave reflector for spectrum shaping function design 5′ reflected by itself passes along the inversion optical path. So this example 2 construction is the same as the self-collimation imaging system and the self-collimation dispersion system. The features of the self-collimator concave spectral shaping device synthesizing system are that the structure in optical path in this example 2 is simple, compact and different from the Littrow system. When the backward wave passes through the above CTSI decomposing system 6-2-3-4-5′, this structure in the inversion optical path constitutes the self-collimation CTSI spectrum synthesizing system, which accomplishes the dispersion cancelling function. Described by the inversion optical path, the modulation light from the concave reflector for spectrum shaping function design 5′ passes through the third concave reflector 4, where it is collimated onto the grating 3, which these comprise a dispersion cancelling construction; then, the parallel light from the grating incident into the second concave reflector 2 focused onto the first aperture 6, which constitute a spectrum synthesizing system with the CTSI construction. All these above constitute the whole spectrum synthesizing system, which is noted by the optical path order 5′-4-3-2-6. Via the first concave reflector 1, it is transferred into a parallel light and accomplished the spectrum decomposing, shaping, and synthesizing, and via the ¼ wave plate 7, its polarization rotates 90 degree; then it is reflected fully at the first beam splitter prism 8 to the second beam splitter prism 9 that is perpendicular to the first one for cancelling the stray light of the modulated chirping pulse, then it is sent into the following stage 0′ such as the solid-state amplifier to be amplified. In present invention of device, the modulated light is reflected and modulated by the concave reflector for spectrum shaping function design 5′, its backward wave via the third concave reflector 4 images onto the dispersion system, which this construction features as the self-collimation system. The diffraction light is reflected back along the inversion optical path order and is projected to the dispersion system, making the extra residual dispersion be zero practically. FIG. 9 is a graph schematically illustrating the shaped pulse waveform of spectrum after modulation by the construction in FIGS. 1, 3 and 4. And FIG. 9 illustrates that this self-collimator concave spectral shaping device makes a depression in the centre wavelength of 1053 nm, and the spectrum modulation ratio can be controlled over 60% under the condition that the phase of the reflecting light remains nearly constant.

In the example 2, the a concave reflector for spectrum shaping function design 5′ could be a multilayer dielectric thin film on a concave reflector for spectrum shaping with micro-structures in it, or a concave reflector for spectrum shaping with micro-mirrors structures in it, or a concave liquid crystal light reflector, or a concave reflector for spectrum shaping with a varied line space grating in front of it, or a concave reflector for spectrum shaping with a liquid crystal spatial light modulator in front of it, or a concave reflector for spectrum shaping with micro-electromechanical mirrors, or a continuous deformation concave reflector for spectrum shaping, or a bimorph deformation concave reflector for spectrum shaping, or a concave reflector for spectrum shaping with a prism/waveguide coupling, or a concave reflector for spectrum shaping with a varied line space grating.

Example 3 of the Device

In this example 3, there are those: the grating 3 is the reflective planar blazed grating, which can endure the high power laser damage and can be fabricated in a large caliber. The concave reflector for spectrum shaping function design 5′ is a concave reflector coated a multilayer dielectric thin film with micro-structures in it as a concave functional reflector for spectrum shaping. All the concave reflectors are made in strictly eliminated the chromatic aberration, the spherical aberration, and the comatic aberration, to ensure the maximal deviation between the spectrum image curved surface and the surface of the concave reflector for spectrum shaping function design less than the tolerance of the half focal depth deduced from the Rayleigh's Criterion. The first aperture 6 is an aperture diaphragm, also is the incident aperture, and the output aperture.

FIG. 1 schematically illustrates the structure of a self-collimator concave spectral shaping device embodying the present invention, which the above elements are settled in this optical path construction. In present invent of device, the spatial arrangement of self-collimator concave spectral shaping device is: all the concave reflectors, the dispersion components, and the aperture in the spectrum decomposing system and those in the spectrum synthesizing system formed after the concave reflector for spectrum shaping function design 5′, and all their images are in a vertical planar. That is to say, the spatial arrangement of self-collimator concave spectral shaping device is constructed as a reflective-type vertical imaging construction for the spectroscope system showed in FIGS. 3 and 5. The parameters of the design requirement, the spatial arrangement, and the optical element showed in table 3, which are:

TABLE 3 the parameters of the design requirement, the spatial arrangement, and the optical element Item Parameters Diameter of the incidence Ø3 mm Normal width 105.3 μm Resolution of line dispersion 0.1 nm/mm Distance between 3000 mm the collimation lens and the imaging lens Value of relative aperture 1: 100 Distance between the grating and 2550 mm the collimation lens or the objective lens Incident angle of the grating    66.36385° as the Littrow angle Diameter of Ø30 mm the incident light onto the grating Density of the grating groove 1740 g/mm Fluence of the grating working 0.5 J/cm{circumflex over ( )}2 Size of the reversible grating 3 100 mm × 50 mm × 20 mm Size of the first concave reflector 1 Ø30 mm × 40 mm, R0.6 m* Size of the second concave reflector 2 Ø292 mm × 40 mm, R6 m* Size of the third concave reflector 4 Ø292 mm × 40 mm, R6 m* Size of the centro-symmetric concave reflector 4″ Ø292 mm × 40 mm, R6 m* Size of the concave reflector for 440 mm × 100 mm × 40 mm R6 m* spectrum shaping function design 5′ Bandwidth of the non-apodized spectra of 24 nm the concave reflector for spectrum shaping function design 5′ Diameter of the first aperture 6 270.89 μm Angle ∠012 between the axis and the centre line of 8° the first concave reflector 1 off-axis settled projecting on the horizontal Angle ∠012 between the axis and the centre line of 6° the first concave reflector 1 off-axis settled projecting on the vertical Angle ∠123 between the axis and the centre line of 8° the second concave reflector 2 off-axis settled projecting on the horizontal Angle ∠123 between the axis and the centre line of 6° the second concave reflector 2 off-axis settled projecting on the vertical Angle ∠234 between the incident light and   132.7277° the diffraction light on the reversion grating 3 projecting on the horizontal Angle ∠234 between the incident light and 6° the diffraction light on the reversion grating 3 projecting on the vertical Angle ∠345′ between the axis and the centre line of    8.7335° the third concave reflector 4 off-axis settled projecting on the horizontal Angle ∠345′ between the axis and the centre line of 6° the third concave reflector 4 off-axis settled projecting on the vertical Angle ∠45′4 between the axis and the centre line of 0° the concave functional reflector 5′ off-axis settled Note: *(radius of curvature)

The self-collimator concave spectral shaping device decomposing system: describing in the optical path order, a laser beam from the front-end system of a CPA system passes through the first beam splitter prism 8 for polarization producing, then it passes through the ¼ wave plate 7 as the p-polarized light in Brewster's angle incidence. And then it passes through the first concave reflector 1 and the second concave reflector 2, which constitute the image transfer construction. Then it focuses onto the first aperture 6. Hence the illumination system is composed of the first concave reflector 1, the first aperture 6, and the second concave reflector 2. Here the first aperture becomes the incident aperture of the spectrum shaping structure in example 3. Then the laser beam passes through the second concave reflector 2, where it is transformed into a parallel light, and then it is projected onto the grating 3, which constitutes the collimation system. However, because of the laser illumination, the first aperture 6 substitutes the slit diaphragm in general CTSI system, and serves as the real light source for the following system, which is the boundary of the beam of an incident light entering into the structure of self-collimator concave spectral shaping device. The laser beam from the first aperture 6 passes through the second concave reflector 2, where it is transformed into a parallel light, and then it is projected onto the grating 3, which comprises the dispersion system. After that, the diffraction light passes through the third concave reflector 4 imaging onto the concave reflector for spectrum shaping function design 5′. All these above constitute the whole spectrum decomposing system, which is denoted by the optical path order 6-2-3-4-5′.

The spectrum shaping system of the self-collimator concave spectral shaping device: The concave reflector for spectrum shaping function design 5′ is a concave reflector coated a multilayer dielectric thin film consisting of alternately arranged high reflective and low reflective material with micro-structures in it as a concave functional reflector for spectrum shaping, which makes the spectrum of chirped pulse a depression in the vicinity of the center but keeps the phase of the reflecting light nearly constant. Furthermore, the spectrum shaping system requires that the maximal deviation between the spectrum image surface and the surface of the concave reflector for spectrum shaping function design 5′ is less than the tolerance of the half focal depth, which is deduced from the Rayleigh's Criterion, and requires that the diameter 2 dr′ of the disc of confusion in the focus plane, or the width a′ of the disc of confusion in the direction of the dispersion are less than a certain value a₀ in the surface of the concave reflector for spectrum shaping function design 5′. The FIG. 8 illustrates that: this the concave reflector for spectrum shaping function design 5′ can make a depression in the vicinity of the spectral center to shape the reflective intensity into a designed spectrum distribution, where curve 1 is the incident chirped pulse spectrum, curve 2 is the modulation curve of a multilayer dielectric reflector determined by the microstructure, and curve 3 is the distribution of chirped pulse spectrum after modulation.

The self-collimator concave spectral shaping device synthesizing system: the diffraction light from the concave reflector for spectrum shaping function design 5′ reflected by itself passes along the inversion optical path. So this example 3 construction is the same as the self-collimation imaging system and the self-collimation dispersion system. The features of the self-collimator concave spectral shaping device synthesizing system are that the structure in optical path in this example 3 is simple, compact and different from the Littrow system. When the backward wave passes through the above CTSI decomposing system 6-2-3-4-5′, this structure in the inversion optical path constitutes the self-collimation CTSI spectrum synthesizing system, which accomplishes the dispersion cancelling function. Described by the inversion optical path, the modulation light from the concave reflector for spectrum shaping function design 5′ passes through the third concave reflector 4, where it is collimated onto the grating 3, which these comprise a dispersion cancelling construction; then, the parallel light from the grating incident into the second concave reflector 2 focused onto the first aperture 6, which constitute a spectrum synthesizing system with the CTSI construction. All these above constitute the whole spectrum synthesizing system, which is noted by the optical path order 5′-4-3-2-6. Via the first concave reflector 1, it is transferred into a parallel light and accomplished the spectrum decomposing, shaping and synthesizing, and via the ¼ wave plate 7, its polarization rotates 90 degree; then it is reflected fully at the first beam splitter prism 8 to the second beam splitter prism 9 that is perpendicular to the first one for cancelling the stray light of the modulated chirping pulse, then it is sent into the following stage 0′ such as the solid-state amplifier to be amplified. In present invention of device, the modulated light is reflected and modulated by the concave reflector for spectrum shaping function design 5′, its backward wave via the third concave reflector 4 images onto the dispersion system, which this construction features as the self-collimation system. The diffraction light is reflected back along the inversion optical path order and is projected to the dispersion system, making the extra residual dispersion be zero practically. FIG. 9 is a graph schematically illustrating the shaped pulse waveform of spectrum after modulation by the construction in FIGS. 1, 3 and 5. And FIG. 9 illustrates that this self-collimator concave spectral shaping device makes a depression in the centre wavelength of 1053 nm, and the spectrum modulation ratio can be controlled over 60% under the condition that the phase of the reflecting light remains nearly constant.

In the example 3, the a concave reflector for spectrum shaping function design 5′ could be a multilayer dielectric thin film on a concave reflector for spectrum shaping with micro-structures in it, or a concave reflector for spectrum shaping with micro-mirrors structures in it, or a concave liquid crystal light reflector, or a concave reflector for spectrum shaping with a varied line space grating in front of it, or a concave reflector for spectrum shaping with a liquid crystal spatial light modulator in front of it, or a concave reflector for spectrum shaping with micro-electromechanical mirrors, or a continuous deformation concave reflector for spectrum shaping, or a bimorph deformation concave reflector for spectrum shaping, or a concave reflector for spectrum shaping with a prism/waveguide coupling, or a concave reflector for spectrum shaping with a varied line space grating.

Example 4 of the Device

In this example 4, there are those: the grating 3 is the reflective planar blazed grating, which can endure the high power laser damage and can be fabricated in a large caliber. The concave reflector for spectrum shaping function design 5′ is a concave reflector coated a multilayer dielectric thin film with micro-structures in it as a concave functional reflector for spectrum shaping. All the concave reflectors are made in strictly eliminated the chromatic aberration, the spherical aberration, and the comatic aberration, to ensure the maximal deviation between the spectrum image curved surface and the surface of the concave reflector for spectrum shaping function design less than the tolerance of the half focal depth deduced from the Rayleigh's Criterion. The first aperture 6 is an aperture diaphragm, also is the incident aperture, and the output aperture.

FIG. 1 schematically illustrates the structure of a self-collimator concave spectral shaping device embodying the present invention, which the above elements are settled in this optical path construction. In present invent of device, the spatial arrangement of a self-collimator concave spectral shaping device is: all the concave reflectors, the dispersion components, and the aperture in the spectrum decomposing system and those in the spectrum synthesizing system formed after the concave reflector for spectrum shaping function design 5′, and all their images are in a vertical planar. That is to say, the spatial arrangement of self-collimator concave spectral shaping device is constructed as a reflective-type vertical imaging construction for the spectroscope system showed in FIGS. 3 and 6. The parameters of the design requirement, the spatial arrangement, and the optical element showed in table 4, which are:

TABLE 4 the parameters of the design requirement, the spatial arrangement, and the optical element Item Parameters Diameter of the incidence Ø3 mm Normal width 105.3 μm Resolution of line dispersion 0.1 nm/mm Distance between 3000 mm the collimation lens and the imaging lens Value of relative aperture 1: 100 Distance between the grating and 2550 mm the collimation lens or the objective lens Incident angle of the grating    66.36385° as the Littrow angle Diameter of Ø30 mm the incident light onto the grating Density of the grating groove 1740 g/mm Fluence of the grating working 0.5 J/cm{circumflex over ( )}2 Size of the reversible grating 3 100 mm × 50 mm × 20 mm Size of the first concave reflector 1 Ø30 mm × 40 mm, R0.6 m* Size of the second concave reflector 2 Ø292 mm × 40 mm, R6 m* Size of the third concave reflector 4 Ø292 mm × 40 mm, R6 m* Size of the centro-symmetric concave reflector 4″ Ø292 mm × 40 mm, R6 m* Size of the concave reflector for 440 mm × 100 mm × 40 mm R6 m* spectrum shaping function design 5′ Bandwidth of the non-apodized spectra of 24 nm the concave reflector for spectrum shaping function design 5′ Diameter of the first aperture 6 270.89 μm Angle ∠012 between the axis and the centre line of 8° the first concave reflector 1 off-axis settled projecting on the horizontal Angle ∠012 between the axis and the centre line of 6° the first concave reflector 1 off-axis settled projecting on the vertical Angle ∠123 between the axis and the centre line of 8° the second concave reflector 2 off-axis settled projecting on the horizontal Angle ∠123 between the axis and the centre line of 6° the second concave reflector 2 off-axis settled projecting on the vertical Angle ∠234 between the incident light and   132.7277° the diffraction light on the reversion grating 3 projecting on the horizontal Angle ∠234 between the incident light and 6° the diffraction light on the reversion grating 3 projecting on the vertical Angle ∠345′ between the axis and the centre line of    8.7335° the third concave reflector 4 off-axis settled projecting on the horizontal Angle ∠345′ between the axis and the centre line of 0° the third concave reflector 4 off-axis settled projecting on the vertical Angle ∠45′4 between the axis and the centre line of 0° the concave functional reflector 5′ off-axis settled Note: *(radius of curvature)

The self-collimator concave spectral shaping device decomposing system: describing in the optical path order, a laser beam from the front-end system of a CPA system passes through the first beam splitter prism 8 for polarization producing, then it passes through the ¼ wave plate 7 as the p-polarized light in Brewster's angle incidence. And then it passes through the first concave reflector 1 and the second concave reflector 2, which constitute the image transfer construction. Then it focuses onto the first aperture 6. Hence the illumination system is composed of the first concave reflector 1, the first aperture 6, and the second concave reflector 2. Here the first aperture becomes the incident aperture of the spectrum shaping structure in example 4. Then the laser beam passes through the second concave reflector 2, where it is transformed into a parallel light, and then it is projected onto the grating 3, which constitutes the collimation system. However, because of the laser illumination, the first aperture 6 substitutes the slit diaphragm in general CTSI system, and serves as the real light source for the following system, which is the boundary of the beam of an incident light entering into the structure of self-collimator concave spectral shaping device. The laser beam from the first aperture 6 passes through the second concave reflector 2, where it is transformed into a parallel light, and then it is projected onto the grating 3, which comprises the dispersion system. After that, the diffraction light passes through the third concave reflector 4 imaging onto the concave reflector for spectrum shaping function design 5′. All these above constitute the whole spectrum decomposing system, which is denoted by the optical path order 6-2-3-4-5′.

The spectrum shaping system of the self-collimator concave spectral shaping device: the concave reflector for spectrum shaping function design 5′ is a concave reflector coated a multilayer dielectric thin film consisting of alternately arranged high reflective and low reflective material with micro-structures in it as a concave functional reflector for spectrum shaping, which makes the spectrum of chirped pulse a depression in the vicinity of the center but keeps the phase of the reflecting light nearly constant. Furthermore, the spectrum shaping system requires that the maximal deviation between the spectrum image surface and the surface of the concave reflector for spectrum shaping function design 5′ is less than the tolerance of the half focal depth, which is deduced from the Rayleigh's Criterion, and requires that the diameter 2 dr′ of the disc of confusion in the focus plane, or the width a′ of the disc of confusion in the direction of the dispersion are less than a certain value a₀ in the surface of the concave reflector for spectrum shaping function design 5′. The FIG. 8 illustrates that: this the concave reflector for spectrum shaping function design 5′ can make a depression in the vicinity of the spectral center to shape the reflective intensity into a designed spectrum distribution, where curve 1 is the incident chirped pulse spectrum, curve 2 is the modulation curve of a multilayer dielectric reflector determined by the microstructure, and curve 3 is the distribution of chirped pulse spectrum after modulation.

The self-collimator concave spectral shaping device synthesizing system: the diffraction light from the concave reflector for spectrum shaping function design 5′ reflected by itself passes along the inversion optical path. So this example 4 construction is the same as the self-collimation imaging system and the self-collimation dispersion system. The features of the self-collimator concave spectral shaping device synthesizing system are that the structure in optical path in this example 4 is simple, compact and different from the Littrow system. When the backward wave passes through the above CTSI decomposing system 6-2-3-4-5′, this structure in the inversion optical path constitutes the self-collimation CTSI spectrum synthesizing system, which accomplishes the dispersion cancelling function. Described by the inversion optical path, the modulation light from the concave reflector for spectrum shaping function design 5′ passes through the third concave reflector 4, where it is collimated onto the grating 3, which these comprise a dispersion cancelling construction; then, the parallel light from the grating incident into the second concave reflector 2 focused onto the first aperture 6, which constitute a spectrum synthesizing system with the CTSI construction. All these above constitute the whole spectrum synthesizing system, which is noted by the optical path order 5′-4-3-2-6. Via the first concave reflector 1, it is transferred into a parallel light and accomplished the spectrum decomposing, shaping and synthesizing, and via the ¼ wave plate 7, its polarization rotates 90 degree; then it is reflected fully at the first beam splitter prism 8 to the second beam splitter prism 9 that is perpendicular to the first one for cancelling the stray light of the modulated chirping pulse, then it is sent into the following stage 0′ such as the solid-state amplifier to be amplified. In present invention of device, the modulated light is reflected and modulated by the concave reflector for spectrum shaping function design 5′, its backward wave via the third concave reflector 4 images onto the dispersion system, which this construction features as the self-collimation system. The diffraction light is reflected back along the inversion optical path order and is projected to the dispersion system, making the extra residual dispersion be zero practically. FIG. 9 is a graph schematically illustrating the shaped pulse waveform of spectrum after modulation by the construction in FIGS. 1, 3 and 6. And FIG. 9 illustrates that this self-collimator concave spectral shaping device makes a depression in the centre wavelength of 1053 nm, and the spectrum modulation ratio can be controlled over 60% under the condition that the phase of the reflecting light remains nearly constant.

In the example 4, the a concave reflector for spectrum shaping function design 5′ could be a multilayer dielectric thin film on a concave reflector for spectrum shaping with micro-structures in it, or a concave reflector for spectrum shaping with micro-mirrors structures in it, or a concave liquid crystal light reflector, or a concave reflector for spectrum shaping with a varied line space grating in front of it, or a concave reflector for spectrum shaping with a liquid crystal spatial light modulator in front of it, or a concave reflector for spectrum shaping with micro-electromechanical mirrors, or a continuous deformation concave reflector for spectrum shaping, or a bimorph deformation concave reflector for spectrum shaping, or a concave reflector for spectrum shaping with a prism/waveguide coupling, or a concave reflector for spectrum shaping with a varied line space grating.

Example 5 of the Device

In this example 5, there are those: the grating 3 is the reflective planar blazed grating, which can endure the high power laser damage and can be fabricated in a large caliber. The concave reflector for spectrum shaping function design 5′ is a concave reflector coated a multilayer dielectric thin film with micro-structures in it as a concave functional reflector for spectrum shaping. All the concave reflectors are made in strictly eliminated the chromatic aberration, the spherical aberration, and the comatic aberration, to ensure the maximal deviation between the spectrum image curved surface and the surface of the concave reflector for spectrum shaping function design less than the tolerance of the half focal depth deduced from the Rayleigh's Criterion. The first aperture 6 is an aperture diaphragm, also is the incident aperture, and the output aperture.

FIG. 1 schematically illustrates the structure of a self-collimator concave spectral shaping device embodying the present invention, which the above elements are settled in this optical path construction. In present invent of device, the spatial arrangement of a self-collimator concave spectral shaping device is: all the concave reflectors, the dispersion components, and the aperture in the spectrum decomposing system and those in the spectrum synthesizing system formed after the concave reflector for spectrum shaping function design 5′, and all their images are in a vertical planar. That is to say, this spatial arrangement of self-collimator concave spectral shaping device is constructed as a reflective-type vertical imaging construction for the spectroscope system showed in FIGS. 3 and 7. The parameters of the design requirement, the spatial arrangement, and the optical element showed in table 5, which are:

TABLE 5 the parameters of the design requirement, the spatial arrangement, and the optical element Item Parameters Diameter of the incidence Ø3 mm Normal width 105.3 μm Resolution of line dispersion 0.1 nm/mm Distance between 3000 mm the collimation lens and the imaging lens Value of relative aperture 1: 100 Distance between the grating and 2550 mm the collimation lens or the objective lens Incident angle of the grating    66.36385° as the Littrow angle Diameter of Ø30 mm the incident light onto the grating Density of the grating groove 1740 g/mm Fluence of the grating working 0.5 J/cm{circumflex over ( )}2 Size of the reversible grating 3 100 mm × 50 mm × 20 mm Size of the first concave reflector 1 Ø30 mm × 40 mm, R0.6 m* Size of the second concave reflector 2 Ø292 mm × 40 mm, R6 m* Size of the third concave reflector 4 Ø292 mm × 40 mm, R6 m* Size of the centro-symmetric concave reflector 4″ Ø292 mm × 40 mm, R6 m* Size of the concave reflector for 440 mm × 100 mm × 40 mm R6 m* spectrum shaping function design 5′ Bandwidth of the non-apodized spectra of 24 nm the concave reflector for spectrum shaping function design 5′ Diameter of the first aperture 6 270.89 μm Angle ∠012 between the axis and the centre line of 8° the first concave reflector 1 off-axis settled projecting on the horizontal Angle ∠012 between the axis and the centre line of 6° the first concave reflector 1 off-axis settled projecting on the vertical Angle ∠123 between the axis and the centre line of 8° the second concave reflector 2 off-axis settled projecting on the horizontal Angle ∠123 between the axis and the centre line of 6° the second concave reflector 2 off-axis settled projecting on the vertical Angle ∠234 between the incident light and 0° the diffraction light on the reversion grating 3 projecting on the horizontal Angle ∠234 between the incident light and 6° the diffraction light on the reversion grating 3 projecting on the vertical Angle ∠345′ between the axis and the centre line of    8.7335° the third concave reflector 4 off-axis settled projecting on the horizontal Angle ∠345′ between the axis and the centre line of 0° the third concave reflector 4 off-axis settled projecting on the vertical Angle ∠45′4 between the axis and the centre line of 0° the concave functional reflector 5′ off-axis settled Note: *(radius of curvature)

The self-collimator concave spectral shaping device decomposing system: describing in the optical path order, a laser beam from the front-end system of a CPA system passes through the first beam splitter prism 8 for polarization producing, then it passes through the ¼ wave plate 7 as the p-polarized light in Brewster's angle incidence. And then it passes through the first concave reflector 1 and the second concave reflector 2, which constitute the image transfer construction. Then it focuses onto the first aperture 6. Hence the illumination system is composed of the first concave reflector 1, the first aperture 6, and the second concave reflector 2. Here the first aperture becomes the incident aperture of the spectrum shaping structure in example 5. Then the laser beam passes through the second concave reflector 2, where it is transformed into a parallel light, and then it is projected onto the grating 3, which constitutes the collimation system. However, because of the laser illumination, the first aperture 6 substitutes the slit diaphragm in general CTSI system, and serves as the real light source for the following system, which is the boundary of the beam of an incident light entering into the structure of self-collimator concave spectral shaping device. The laser beam from the first aperture 6 passes through the second concave reflector 2, where it is transformed into a parallel light, and then it is projected onto the grating 3, which comprises the dispersion system. After that, the diffraction light passes through the third concave reflector 4 imaging onto the concave reflector for spectrum shaping function design 5′. All these above constitute the whole spectrum decomposing system, which is denoted by the optical path order 6-2-3-4-5′.

The spectrum shaping system of the self-collimator concave spectral shaping device: the concave reflector for spectrum shaping function design 5′ is a concave reflector coated a multilayer dielectric thin film consisting of alternately arranged high reflective and low reflective material with micro-structures in it as a concave functional reflector for spectrum shaping, which makes the spectrum of chirped pulse a depression in the vicinity of the center but keeps the phase of the reflecting light nearly constant. Furthermore, the spectrum shaping system requires that the maximal deviation between the spectrum image surface and the surface of the concave reflector for spectrum shaping function design 5′ is less than the tolerance of the half focal depth, which is deduced from the Rayleigh's Criterion, and requires that the diameter 2 dr′ of the disc of confusion in the focus plane, or the width a′ of the disc of confusion in the direction of the dispersion are less than a certain value a₀ in the surface of the concave reflector for spectrum shaping function design 5′. The FIG. 8 illustrates that: this the concave reflector for spectrum shaping function design 5′ can make a depression in the vicinity of the spectral center to shape the reflective intensity into a designed spectrum distribution, where curve 1 is the incident chirped pulse spectrum, curve 2 is the modulation curve of a multilayer dielectric reflector determined by the microstructure, and curve 3 is the distribution of chirped pulse spectrum after modulation.

The self-collimator concave spectral shaping device synthesizing system: the diffraction light from the concave reflector for spectrum shaping function design 5′ reflected by itself passes along the inversion optical path. So this example 5 construction is the same as the self-collimation imaging system and the self-collimation dispersion system. The features of the self-collimator concave spectral shaping device synthesizing system are that the structure in optical path in this example 5 is simple, compact and different from the Littrow system. When the backward wave passes through the above CTSI decomposing system 6-2-3-4-5′, this structure in the inversion optical path constitutes the self-collimation CTSI spectrum synthesizing system, which accomplishes the dispersion cancelling function. Described by the inversion optical path, the modulation light from the concave reflector for spectrum shaping function design 5′ passes through the third concave reflector 4, where it is collimated onto the grating 3, which these comprise a dispersion cancelling construction; then the parallel light from the grating incident into the second concave reflector 2 focused onto the first aperture 6, which constitute a spectrum synthesizing system with the CTSI construction. All these above constitute the whole spectrum synthesizing system, which is noted by the optical path order 5′-4-3-2-6. Via the first concave reflector 1, it is transferred into a parallel light and accomplished the spectrum decomposing, shaping and synthesizing, and via the ¼ wave plate 7, its polarization rotates 90 degree; then it is reflected fully at the first beam splitter prism 8 to the second beam splitter prism 9 that is perpendicular to the first one for cancelling the stray light of the modulated chirping pulse, then it is sent into the following stage 0′ such as the solid-state amplifier to be amplified. In present invention of device, the modulated light is reflected and modulated by the concave reflector for spectrum shaping function design 5′, its backward wave via the third concave reflector 4 images onto the dispersion system, which this construction features as the self-collimation system. The diffraction light is reflected back along the inversion optical path order and is projected to the dispersion system, making the extra residual dispersion be zero practically. FIG. 9 is a graph schematically illustrating the shaped pulse waveform of spectrum after modulation by the construction in FIGS. 1, 3 and 7. And FIG. 9 illustrates that this self-collimator concave spectral shaping device makes a depression in the centre wavelength of 1053 nm, and the spectrum modulation ratio can be controlled over 60% under the condition that the phase of the reflecting light remains nearly constant.

In the example 5, the a concave reflector for spectrum shaping function design 5′ could be a multilayer dielectric thin film on a concave reflector for spectrum shaping with micro-structures in it, or a concave reflector for spectrum shaping with micro-mirrors structures in it, or a concave liquid crystal light reflector, or a concave reflector for spectrum shaping with a varied line space grating in front of it, or a concave reflector for spectrum shaping with a liquid crystal spatial light modulator in front of it, or a concave reflector for spectrum shaping with micro-electromechanical mirrors, or a continuous deformation concave reflector for spectrum shaping, or a bimorph deformation concave reflector for spectrum shaping, or a concave reflector for spectrum shaping with a prism/waveguide coupling, or a concave reflector for spectrum shaping with a varied line space grating. 

1. A self-collimator concave spectral shaping device for chirped-pulse-amplification (CPA): of which the features are the comprising: in the optical path order, the first beam splitter prism (8), the second beam splitter prism (9), and the ¼ wave plate (7); and the first concave reflector (1), the first aperture (6), and the second concave reflector (2), which these (1)-(6)-(2) constitute a illumination system; and, the first aperture (6), the second concave reflector (2), the grating (3), the third concave reflector (4) and the concave reflector for spectrum shaping function design (5′), which these (6)-(2)-(3)-(4)-(5′) constitute a spectrum decomposing system with Czerny-Turner Spectroscope Instrument (CTSI) construction for self-collimator concave spectral shaping device; in addition, the concave reflector for spectrum shaping function design (5′) constitutes a spectrum shaping system; furthermore, the concave reflector for spectrum shaping function design (5′), the third concave reflector (4), the grating (3), the second concave reflector (2), and the first aperture (6), which these (5′)-(4)-(3)-(2)-(6) constitute a spectrum synthesizing system with CTSI construction for self-collimator concave spectral shaping device; of which the features are the processing: a laser beam from the front-end system (0) of a CPA system passes through the first beam splitter prism for polarization producing; via the ¼ wave plate and the first concave reflector, then it passes through the first concave reflector, which transferring the laser beam into a parallel light; As mentioned above, it passes through the spectrum decomposing system, the spectrum shaping system and the spectrum synthesizing system for self-collimator concave spectral shaping device, which accomplish the spectrum decomposing, the spectrum shaping, and the spectrum synthesizing of the chirped pulse; then it passes through the ¼ wave plate, its polarization rotates 90 degree; after that, it is reflected fully by the first beam splitter prism to the second beam splitter prism for a polarization producing of the modulated chirped pulse, and sent into the following stage such as the solid-state amplifier to amplification.
 2. The self-collimator concave spectral shaping device as recited in claim 1, of which the features are: wherein the grating (3) is the reflective planar blazed grating.
 3. The self-collimator concave spectral shaping device as recited in claim 1, of which the features are: wherein all the concave reflectors are made with the chromatic aberration, the spherical aberration, the comatic aberration, the astigmatism and the field curvature eliminated strictly in the whole working frequency bandwidth, to ensure the maximized deviation between the spectrum image curved surface and the concave reflector for spectrum shaping function design less than the tolerance of the half focal depth.
 4. The self-collimator concave spectral shaping device as recited in claim 1, of which the features are: as the beam is reflected by the concave reflector for spectrum shaping function design (5′), its backward wave passing along the inversion optical path, so making the concave spectral shaping device constructed as the self-collimator system.
 5. The self-collimator concave spectral shaping device as recited in claim 1, of which the features are: wherein all the concave reflectors are constructed a symmetrical imaging system relative to the dispersion component, or are constructed an asymmetrical imaging system relative to the dispersion component for compensating the aberration of the image.
 6. The self-collimator concave spectral shaping device as recited in claim 1, of which the features are: wherein the first aperture (6) is the aperture diaphragm in the real confocal telescope, which constructed as an illumination system and as an image transfer system; wherein the illumination system ensures that the normal width is suitable for the coherence and phase consisted conditions for a incident light, the distribution of a laser beam obtained from the front-end system of a CPA system do not changed in the spatial and temporal domain, the relative aperture in the illumination system must matched with the relative apertures in the dispersion system and in the imaging system, and the clear aperture can fill the caliber of the dispersion element; wherein the first aperture (6) is the aperture diaphragm in the real confocal telescope, which must satisfy the normal width a₀ condition for a diaphragm, or the diffraction half width a₀ condition for the spectrum decomposing system and the spectrum synthesizing system, and which must have the capability passes through the light with all the frequencies within the chirped laser pulse bandwidth.
 7. The self-collimator concave spectral shaping device as recited in claim 1, of which the features are: wherein the a concave reflector for spectrum shaping function design (5′) could be a multilayer dielectric thin film on a concave reflector for spectrum shaping with micro-structures in it, or a concave reflector for spectrum shaping with micro-mirrors structures in it, or a concave liquid crystal light reflector, or a concave reflector for spectrum shaping with a varied line space grating in front of it, or a concave reflector for spectrum shaping with a liquid crystal spatial light modulator in front of it, or a concave reflector for spectrum shaping with micro-electromechanical mirrors, or a continuous deformation concave reflector for spectrum shaping, or a bimorph deformation concave reflector for spectrum shaping, or a concave reflector for spectrum shaping with a prism/waveguide coupling, or a concave reflector for spectrum shaping with a varied line space grating.
 8. The self-collimator concave spectral shaping device as recited in claim 1, of which the features are: wherein the first beam splitter prism (8) is fully perpendicular to the second beam splitter prism (9).
 9. The self-collimator concave spectral shaping device as recited in claim 1, of which the features are: wherein all the concave reflectors in the spectrum decomposing system and all the concave reflectors in the spectrum synthesizing system are constructed as a reflective-type horizontal imaging system relative to the dispersion component for the spectroscope system, or are constructed as a reflective-type vertical imaging system relative to the dispersion component for the spectroscope system.
 10. The self-collimator concave spectral shaping device as recited in claim 1, of which the features are: wherein the spectrum decomposing system and the spectrum synthesizing system are constructed as a reflective-type horizontal imaging and shaping system relative to the concave reflector for spectrum shaping function design (5′) for the spectroscope system, or are constructed as a reflective-type vertical imaging and shaping system relative to the concave reflector for spectrum shaping function design (5′) for the spectroscope system. 